BACKGROUND OF THE INVENTION
1. Field of the Invention
[0001] The present invention relates to a semiconductor device, and particularly to a semiconductor
device including a vertical Hall element which detects a horizontal magnetic field.
2. Background Art
[0002] A Hall element has been used for various applications because of possible non-contact
detection of position and angle as a magnetic sensor. Of these, a magnetic sensor
using a horizontal Hall element detecting a magnetic field component perpendicular
to the surface of the semiconductor substrate has generally been known well, and various
magnetic sensors each using a vertical Hall element detecting a magnetic field component
parallel to the surface of the semiconductor substrate have also been proposed. Further,
there has also been proposed a magnetic sensor which makes two-dimensional or three-dimensional
detection of a magnetic field by combining a horizontal Hall element and a vertical
Hall element.
[0003] Characteristics variation of a vertical Hall element is, however, large since sensitivity
and offset voltage characteristics of the vertical Hall element is apt to be affected
by production variation as compared with the horizontal Hall element.
[0004] In order to calibrate such characteristics variation, there has been disclosed in
U.S. Patent No. 9116192, a method for estimation of the sensitivity of the Hall element in which a current
flows through an excitation conductor disposed in the vicinity of a vertical Hall
element to thereby generate a calibration magnetic field having a predetermined magnetic
flux density in the position of the Hall element. That is, the actual sensitivity
of the Hall element is estimated by changing the magnetic flux density of the calibration
magnetic field and measuring a change in a Hall voltage supplied from the Hall element
during the application of the calibration magnetic field.
[0005] Further, there has been illustrated in FIG. 1 of
U.S. Patent No. 9116192, a structure in which the horizontal distance between the center of an excitation
conductor and the center of a vertical Hall element is separated, i.e., the center
of the excitation conductor is shifted in a horizontal direction from the center of
the vertical Hall element. It is thus possible to suppress the vertical Hall element
from being affected by variation in a magnetic field intensity generated by the excitation
conductor due to variation in the width of the excitation conductor, etc. by a process
fluctuation during the manufacture of a semiconductor device.
[0007] That is, the distance between the vertical Hall element and the excitation conductor
is enlarged by separating the horizontal distance between the center of the excitation
conductor and the center of the vertical Hall element. Since the magnetic field intensity
generated by the current flowing through the excitation conductor is inversely proportional
to the distance from the excitation conductor, the intensity of the calibration magnetic
field applied to the vertical Hall element becomes small when the distance between
the vertical Hall element and the excitation conductor becomes large.
[0008] A change in the Hall voltage supplied from the vertical Hall element becomes small
when the intensity of the calibration magnetic field applied to the vertical Hall
element becomes small. It is thus possible to suppress variation in the intensity
of the calibration magnetic field applied to the vertical Hall element, but since
the intensity of the calibration magnetic field reduces, accuracy in estimating actual
sensitivity of the vertical Hall element degrades as a result.
[0009] The current flowing through the excitation conductor is accordingly increased to
enlarge the intensity of the calibration magnetic field applied to the vertical Hall
element: the amount of heat generation from the excitation conductor thereby increases.
In
U.S. Patent No. 9116192, the center of the excitation conductor is shifted in the horizontal direction from
the center of the vertical Hall element, whereby the excitation conductor approaches
to a peripheral circuit such as a circuit which processes an output signal from the
vertical Hall element, a circuit to supply a signal to the vertical Hall element,
or the like, and which are disposed around the vertical Hall element. Temperature
distribution therefore occurs in the peripheral circuit due to the heat generation
of the excitation conductor. The characteristics of the peripheral circuit thereby
fluctuate, thus leading to degradation of the accuracy in estimating actual characteristics
of the vertical Hall element.
[0010] Incidentally, increasing the distance between the excitation conductor and the peripheral
circuit may suppress the generation of the temperature distribution in the peripheral
circuit, but may not be realistic because of heading against the miniaturization of
the semiconductor device.
SUMMARY OF THE INVENTION
[0011] The present invention therefore aims to provide a semiconductor device capable of
suppressing heating of an excitation conductor from affecting a peripheral circuit,
enlarging the intensity of a calibration magnetic field received by a vertical Hall
element, and thereby performing high-accuracy calibration of the vertical Hall element.
[0012] A semiconductor device according to one aspect of the present invention is provided
which includes a semiconductor substrate of a first conductivity type, a vertical
Hall element provided on the semiconductor substrate, and an excitation conductor
provided directly above the vertical Hall element with an intermediation of an insulating
film. The vertical Hall element includes a semiconductor layer of a second conductivity
type provided on the semiconductor substrate, and a plurality of electrodes each constituted
from a high-concentration second conductivity type impurity region and provided on
the surface of the semiconductor layer along a straight line. A ratio W
C/W
H between a width W
C of the excitation conductor and a width W
H of each of the plurality of electrodes satisfying an inequality 0.3≤W
C/W
H≤1.0.
[0013] According to the present invention, the excitation conductor is disposed directly
above the vertical Hall element, and the ratio W
C/W
H between the width W
C of the excitation conductor and the width W
H of each electrode of the vertical Hall element is assumed to be less than or equal
to 1.0, whereby a peripheral circuit such as a circuit processing an output signal
from the vertical Hall element, a circuit to supply a signal to the vertical Hall
element, or the like, and the excitation conductor can be disposed so as not to approach
each other. Also, since it is possible to suppress an increase in the amount of heat
generation from the excitation conductor by setting W
C/W
H to be greater than or equal to 0.3, occurrence of a temperature distribution in the
peripheral circuit can be prevented. Further, the intensity of a calibration magnetic
field received by the vertical Hall element can be enlarged by disposing the excitation
conductor directly above the vertical Hall element. It is thus possible to enlarge
the intensity of the calibration magnetic field applied to the vertical Hall element
and perform calibration of the vertical Hall element with high accuracy while suppressing
the amount of heat generation from the excitation conductor.
BRIEF DESCRIPTION OF THE DRAWINGS
[0014] Embodiments of the present invention will now be described by way of further example
only and with reference to the accompanying drawings, in which:
FIG. 1A is a plan view of a semiconductor device having a vertical Hall element according
to an embodiment of the present invention, and FIG. 1B is a sectional view taken along
line L-L' of FIG. 1A;
FIG. 2 is a graph illustrating a result in which a relation between a ratio (WC/WH) between a width WC of an excitation conductor and a width WH of each electrode of the vertical Hall element and an increase in the temperature
of the excitation conductor when the excitation conductor generates a magnetic field
having a magnetic flux density of 2mT is simulated by changing a ratio (h/WH) between a distance h from the center of the vertical Hall element in a substrate
depthwise direction to the excitation conductor and the width WH of each electrode of the vertical Hall element; and
FIG. 3 is a graph illustrating a result in which a relation between the ratio (WC/WH) between the width WC of the excitation conductor and the width WH of each electrode of the vertical Hall element and a magnetic flux density (B/I)
applied to the vertical Hall element per unit current flowing through the excitation
conductor is simulated by changing the ratio (h/WH) between the distance h from the center of the vertical Hall element in a substrate
depthwise direction to the excitation conductor 200 and the width WH of each electrode of the vertical Hall element.
DESCRIPTION OF THE EMBODIMENTS
[0015] Embodiments of the present invention will hereinafter be described in detail with
reference to the accompanying drawings.
[0016] FIG. 1 is a view for describing a semiconductor device having a vertical Hall element
according to the embodiment of the present invention in which FIG. 1A is a plan view,
and FIG. 1B is a sectional view taken along line L-L' of FIG. 1A.
[0017] As illustrated in FIG. 1, the semiconductor device according to the present embodiment
includes a semiconductor substrate 10 of a P type (first conductivity type), a P-type
element isolation diffusion layer 20, a vertical Hall element 100 provided on the
semiconductor substrate 10, an insulating film 30 provided on the vertical Hall element
100, and an excitation conductor 200 provided on the insulating film 30.
[0018] The vertical Hall element 100 is constituted from an N type (second conductivity
type) semiconductor layer 101 serving as a magnetism sensing part which is provided
on the semiconductor substrate 10, and electrodes 111 through 115 each constituted
from an N type impurity region are provided on the surface of the semiconductor layer
101 along a straight line. The electrodes 111 through 115 have a rectangular shape
and a common width W
H and are provided in parallel to each other.
[0019] The element isolation diffusion layer 20 electrically isolates the vertical Hall
element 100 from other regions (not illustrated) on the semiconductor substrate 10.
[0020] Elements such as transistors provided in other regions on the semiconductor substrate
10 are electrically isolated from the vertical Hall element 100 by the element isolation
diffusion layer 20. The elements constitute a circuit which processes an output signal
from the vertical Hall element 100, a circuit which supplies a signal to the vertical
Hall element 100, or a circuit which compensates the characteristics of the vertical
Hall element 100 by a calibration magnetic field, or the like (hereinafter called
a "peripheral circuit").
[0021] The excitation conductor 200 has a linear shape and is provided directly above the
vertical Hall element 100 with an intermediation of the insulating film 30 in such
a manner that a longitudinal center line of the excitation conductor 200 and a longitudinal
center line of the semiconductor layer (magnetism sensing part) 101 of the vertical
Hall element 100 coincide. The distance between the excitation conductor 200 and the
vertical Hall element 100 thereby becomes the smallest, and hence the intensity of
the calibration magnetic field received by the vertical Hall element 100 can be made
larger. Further, the uniform calibration magnetic field can be supplied to the whole
vertical Hall element 100.
[0022] Then, in the present embodiment, the ratio W
C/W
H between the width W
C of the excitation conductor 200 on the vertical Hall element 100 and the width W
H of each of the electrodes 111 through 115 of the vertical Hall element 100 satisfies
an inequality 0.3≤W
C/W
H≤1.0. A description will be made below as to the reason why such an inequality is
taken.
[0023] As the calibration magnetic field applied to the vertical Hall element 100 and generated
from the excitation conductor 200 becomes small, a change in the Hall voltage supplied
from the vertical Hall element 100 becomes small, thereby degrading the accuracy for
estimation of actual sensitivity of the vertical Hall element 100. It is therefore
preferable to apply the calibration magnetic field of 2 to 3mT or more.
[0024] With the above in view, FIG. 2 illustrates a graph of a result in which the relation
between the ratio W
C/W
H and an increase in the temperature of the excitation conductor 200 when the excitation
conductor 200 generates a magnetic field having a magnetic flux density of 2mT is
simulated. Here, W
C/W
H is a ratio between the width W
C of the excitation conductor 200 and the width W
H of each of the electrodes 111 through 115 of the vertical Hall element 100 and the
simulation is made by changing a ratio h/W
H between a distance h from the center of the vertical Hall element 100, which is mainly
constituted from the semiconductor layer 101, in a substrate depthwise direction to
the excitation conductor 200 and the width W
H of each of the electrodes 111 through 115 of the vertical Hall element 100.
[0025] It is understood from the graph of FIG. 2 that the increase in the temperature of
the excitation conductor 200 abruptly becomes large upon the ratio W
C/W
H between the width W
C of the excitation conductor and the width W
H of each of the electrodes 111 through 115 of the vertical Hall element reaching less
than or equal to 0.3. Incidentally, FIG. 2 illustrates the simulation result in which
the excitation conductor 200 generates the magnetic field having the magnetic flux
density of 2mT as an example, but it has been confirmed that even when the excitation
conductor 200 generates a magnetic field having a magnetic flux density of 3mT or
more, the shape of the graph becomes similar, and an increase in the temperature of
the excitation conductor 200 abruptly becomes large upon W
C/W
H reaching less than or equal to 0.3.
[0026] Accordingly, by setting the ratio W
C/W
H between the width W
C of the excitation conductor and the width W
H of each of the electrodes 111 through 115 of the vertical Hall element to be greater
than or equal to 0.3, it is possible to suppress the occurrence of a temperature distribution
in the peripheral circuit upon applying a current to the excitation conductor 200
to apply a calibration magnetic field of more than 2 to 3mT to the vertical Hall element
100.
[0027] On the other hand, the peripheral circuit and the excitation conductor 200 approach
each other when the width W
C of the excitation conductor 200 becomes larger than the width W
H of each of the electrodes 111 through 115 of the vertical Hall element 100. That
is, the peripheral circuit becomes vulnerable to the heat generation from the excitation
conductor 200, and the accuracy of estimating the actual characteristics of the vertical
Hall element 100 is degraded. It is thus preferable that in order to prevent the excitation
conductor 200 from approaching the peripheral circuit, the width W
C of the excitation conductor 200 is not made larger than the width of each of the
electrodes 111 through 115 of the vertical Hall element 100, i.e., the ratio W
C/W
H between the width W
C of the excitation conductor and the width W
H of each of the electrodes 111 through 115 of the vertical Hall element is set to
be less than or equal to 1.0.
[0028] FIG. 3 is a graph illustrating a result in which a relation between the ratio W
C/W
H and a magnetic flux density (B/I) applied to the vertical Hall element 100 per unit
current flowing through the excitation conductor 200 is simulated. Here, W
C/W
H is a ratio between the width W
C of the excitation conductor 200 and the width W
H of each of the electrodes 111 through 115 of the vertical Hall element 100, and the
simulation is made by changing the ratio h/W
H between the distance h from the center of the vertical Hall element 100 in a depthwise
direction of the substrate to the excitation conductor 200 and the width W
H of each of the electrodes 111 through 115 of the vertical Hall element 100.
[0029] It is understood from the graph of FIG. 3 that the magnetic flux density (B/I) applied
to the vertical Hall element 100 per unit current flowing through the excitation conductor
200 becomes small as the ratio h/W
H between the distance h from the center of the vertical Hall element 100 in the depthwise
direction of the substrate to the excitation conductor 200 and the width W
H of each of the electrodes 111 through 115 of the vertical Hall element 100 is made
large. Hence the ratio h/W
H is preferably as small as possible.
[0030] Further, as can be seen from FIG. 2, the increase in the temperature of the excitation
conductor 200 becomes large as the ratio h/W
H between the distance h from the center of the vertical Hall element 100 in the substrate
depthwise direction to the excitation conductor and the width W
H of each of the electrodes 111 through 115 of the vertical Hall element 100 is made
larger.
[0031] That is, as the distance h from the center of the vertical Hall element 100 in the
substrate depthwise direction to the excitation conductor 200 becomes large, more
current must flow to the excitation conductor 200 in order to apply a required calibration
magnetic field to the vertical Hall element 100. The increase in the temperature of
the excitation conductor 200 therefore becomes large, thereby affecting the peripheral
circuit.
[0032] Accordingly, even if the ratio W
C/W
H between the width W
C of the excitation conductor 200 and the width W
H of each of the electrodes 111 through 115 of the vertical Hall element 100 is within
a range which satisfies 0.3≤W
C/W
H≤1.0, the increase in the temperature of the excitation conductor 200 is preferably
5°C or less to suppress affection to the peripheral circuit.
[0033] From FIG. 3, consequently, the ratio h/W
H between the distance h from the center of the vertical Hall element 100 in the substrate
depthwise direction to the excitation conductor 200 and the width W
H of each of the electrodes 111 through 115 of the vertical Hall element 100 is preferably
set to 0.4 or less at which the increase in the temperature of the excitation conductor
200 becomes 5°C or less in the range in which the ratio W
C/W
H between the width W
C of the excitation conductor and the width W
H of each of the electrodes 111 through 115 of the vertical Hall element is 0.3 or
more.
[0034] Incidentally, in a process of forming the vertical Hall element 100, forming the
insulating film 30 thereon, and then forming wirings to electrically connect the plurality
of elements such as the transistors constituting the peripheral circuit to each other,
the excitation conductor 200 can be formed simultaneously with the wirings. According
to the present embodiment, it is therefore possible to form the excitation conductor
200 without increasing a manufacturing process.
[0035] Further, even if, for example, when W
C/W
H is designed to be 0.5, variation occurs in the width of the excitation conductor
200 due to variations in the manufacturing process so that W
C/W
H becomes 0.5+α or 0.5-α, a change in the magnetic flux density relative to its change
is small as can be seen from FIG. 3 because the ratio W
C/W
H between the width W
C of the excitation conductor 200 and the width W
H of each of the electrodes 111 through 115 of the vertical Hall element 100 is 0.3≤W
C/W
H≤1.0. That is, even if the width of the excitation conductor 200 or the like varies
due to the variations in the manufacturing process, a fluctuation in the intensity
of the magnetic field generated from the excitation conductor 200 can be suppressed
to be small.
[0036] Here, resistivity of the excitation conductor 200 is preferably as low as possible
to reduce the amount of heat generation, e.g., the excitation conductor 200 is preferably
formed of Al or the like. Further, the excitation conductor 200 is preferably as thick
as possible to reduce the amount of heat generation, e.g., desirably 0.5µm or more.
[0037] A description will next be made as to a method of compensating the characteristics
of the vertical Hall element 100 in the semiconductor device according to the present
embodiment by the calibration magnetic field.
[0038] A current flow through the excitation conductor 200 generates a calibration magnetic
field Bc having a predetermined magnetic flux density indicated by a dotted line around
the excitation conductor 200 as illustrated in FIG. 1B, whereby the calibration magnetic
field Bc is applied to the vertical Hall element 100 in a horizontal direction. At
this time, the predetermined magnetic flux density is preferably set to be a few mT
or so.
[0039] In a state in which the calibration magnetic field Bc is applied, a drive current
is supplied to the electrode serving as a drive current supply electrode, of the electrodes
111 through 115 of the vertical Hall element 100. Since the drive current receives
the Lorentz force caused by the calibration magnetic field Bc, a potential difference
is generated between the electrodes serving as Hall voltage output electrodes, of
the electrodes 111 through 115 of the vertical Hall element 100, whereby this potential
difference is obtained as a Hall voltage. Specifically, a Hall voltage is provided
between the electrodes 112 and 114 by, for example, supplying the drive current to
the electrodes 111, 113, and 115 in such a manner that a current flows from the electrode
113 to the electrodes 111 and 115.
[0040] The drive current and the gain of an amplifier connected to the output of the vertical
Hall element 100, etc. are adjusted based on the Hall voltage obtained in this manner,
an offset voltage remaining after calculation of a plurality of Hall voltages obtained
by changing the direction of supplying the drive current by a spinning current method,
etc., thereby carrying out compensation of the characteristics of the vertical Hall
element 100. It is thus possible to achieve a semiconductor device having the vertical
Hall element 100 which suppresses variation in its characteristics with high accuracy.
[0041] The embodiment of the present invention has been described above, but the present
invention is not limited to the above embodiment. It is needless to say that various
changes can be made thereto within the scope of the present invention.
[0042] For example, in the above embodiment, the excitation conductor 200 is illustrated
in the single layer, but the thickness of the excitation conductor 200 may be increased
as a whole by using a multilayer wiring to increase the whole thickness of the excitation
conductor 200.
[0043] Also, there has been illustrated the example using Al or the like as the excitation
conductor 200, but a conductor such as polysilicon or the like may be used.
[0044] Further, the first conductivity type and the second conductivity type have been described
as the P type and the N type respectively, but they may be replaced with each other
so that the first conductivity type functions as the N type and the second conductivity
type functions as the P type.
[0045] Furthermore, the above embodiment has illustrated the example in which the vertical
Hall element 100 has the five electrodes, but the vertical Hall element 100 may have
three in total including two for the supply of the drive current and one for the output
of the Hall voltage, or more.